Serena Margadonna

Bulk superconductivity at 38 K in a molecular system

\ensuremath{\alpha}\text{-FeSe}

Crystal structure of the new FeSe1−x superconductor

with the PbO structure is a key member of the family of high-

Strong Electron Correlations in the Normal State of the Iron-Based FeSe0.42Te0.58 Superconductor Observed by Angle-Resolved Photoemission Spectroscopy

{T}_{c}

Temperature-induced valence transition and associated lattice collapse in samarium fulleride

iron pnictide and chalcogenide superconductors, as while it possesses the basic layered structural motif of edge-sharing distorted

Crystal structure and phase transitions across the metal-superconductor boundary in the SmFeAsO 1 − x F x ( 0 ≤ x ≤ 0.20 ) family

{\text{FeSe}}_{4}

Phase separation in carbon-doped MgB2 superconductors

tetrahedra, it lacks interleaved ion spacers or charge-reservoir layers. We find that the application of hydrostatic pressure first rapidly increases

Unusual polymerization in the Li4C60 fulleride

{T}_{c}

Influence of the Nd 4ƒ states on the magnetic behavior and the electric field gradient of the oxypnictides superconductors NdFeAsO1-xFx

which attains a broad maximum of 37 K at

Vibrational Spectroscopy of Superconducting MgB2 by Neutron Inelastic Scattering

\ensuremath{\sim}7\text{ }\text{GPa}